The q-deformed boson gas at finite temperature is investigated for the
quantum deformation parameter q to be complex (s = ln q = a + ib). It
is shown that the real part of the energy density distribution corres
ponds to the Planck energy density distribution for a suitable range o
f the parameter b, which restricts the maximum number of quantum state
s in the model of the system. The spectra of q-oscillator are differen
t for different (a, b)-values. The classical dimensionless constant, c
haracterizing the Wien shift law, is presented as a function of (a, b)
and, in the spirit of the theory of q-deformed boson gas, it is possi
ble to interpret it as the radiation of a non-ideal black-body or a re
al body. The role of the imaginary part of oscillator energy is also s
tudied.